WO1986004997A1

WO1986004997A1 - Interferometers

Info

Publication number: WO1986004997A1
Application number: PCT/GB1986/000101
Authority: WO
Inventors: Keith Gardner; Robert James Longman; Robert Martin Pettigrew; Walter Thompson Welford
Original assignee: Keith Gardner; Robert James Longman; Robert Martin Pettigrew; Walter Thompson Welford
Priority date: 1985-02-25
Filing date: 1986-02-25
Publication date: 1986-08-28
Also published as: EP0193381A1; EP0193381B1; DE3665778D1; US4802736A

Abstract

An interferometer which comprises: (1) a single, coherent light source; (2) a first converging lens positioned on the optical axis of said coherent light source; (3) a beam-splitting arrangement positioned on said optical axis and spaced from said first converging lens by a distance greater than the focal length of said lens; (4) a second converging lens positioned on said optical axis to receive and to focus the two beams emanating in use from the beam-splitting arrangement; and (5) a mirror arrangement positioned so that the beams focussed by said second converging lens impinge on the mirror system and so that the reflected beams are brought to intersect at a focal point and with a large angle between the principal rays of the two beams.

Description

" INTERFEROMETERS "

This invention relates to interferometers and in particular to interferometers for use in generating closely spaced interference fringes focussed accurately on an object, typically a glass disk carrying a thin layer of a photoresist.

Optical data storage systems are known which use, as the storage member, a disk carrying a radiation-sensitive layer which has a regular textured surface pattern, for example in the form of a plurality of grooves or an array of protuberances. Optical data storage disks of this type are described, for example, in European Patent Publication No.0107379. The required dimensions of the textured surface pattern in this and similar optical data storage disks are on a minute scale and hence problems may be experienced in generating a master from which such optical data storage disks may be replicated.

It is known to expose a photoresist to an interference pattern in light of a wavelength to which the photores ist is sens it ive . It is very di f f icult , however, to generate an interference pattern the fringes of which are concentric circles and are spaced apart by one micron or less.

According to the present invention, there is provided an interferometer which comprises: (1) a single, coherent light source; (2) a first converging lens positioned on the optical axis of said coherent light source; (3) a beam-splitting arrangement positioned on said optical axis and spaced from said first converging lens by a distance greater than the focal length of said lens; (4) a second converging lens positioned on said optical axis to receive and to focus the two beams emanating in use from the beam-splitting arrangement ; and ( 5 ) a mirror arrangement pos it ioned so that the beams focussed by said second converging lens impinge on the mirror system and so that the reflected beams are brought to intersect at a focal point and with a large angle between the principal rays of the two beams.

Preferably, the beam-splitting arrangement comprises a Wollaston double image prism followed by a polarising arrangement. The coherent light source is conve i tly a laser generating light of wavelength about 450 n less. The first converging lens preferably has a focal length of about 40-50 mm and the second converging lens can conveniently be a microscope objective. For example, if a laser beam of wavelength 450 nm is focussed by a microscope objective of numerical aperture 0.25, the width of the beam at half intensity will be about 900 nm and if the beam splitting arrangement and mirror arrangement cause two such beams to intersect at 90º, they will form at the focal point straight fringes with a spacing of about 300 nm. It is preferable for the angle of intersection of the two beams to be at least 45º, and more preferably at least 90º. The invention will be described further with reference to the accompanying drawings, in which:

FIGURE 1 illustrates schematically an optical system in accordance with the present invention; and

FIGURE 2 is an enlarged ray diagram illustrating the operation of part of the optical system of Figure 1. Referring now to the drawings, a laser (not shown) generates a beam B which is focussed by a first converging lens L of focal length 45 mm to a beam waist at a pinhole A which is 20-25 microns in diameter. A prism R is positioned between lens L. and the pinhole A in the manner shown. The pinhole serves to remove stray light from the laser beam but may be omitted if the laser used is of sufficiently high quality. In any event, the pinhole or beam waist is the object which is to be imaged by the remainder of the optical system.

A first halfwave plate P₁ is positioned between the pinhole A and the beam-splitting arrangement which consists of a Wollaston double image prism W. The halfwave plate P₁ serves to rotate the plane of polarisation of the laser beam so that it is at 45 to the splitting plane of the Wollaston prism W (this plane being the plane of the diagram). The Wollaston prism W may be formed for example of quartz or of calcite; with the former, the prism angle is 63°, while with the latter it is 6.6°. The specified angle should be accurate to within + or -1.2°. A polariser P is set at 45° to the splitting plane in order to select equal intensity components of the same polarisation. A second halfwave plate P₃ serves to rotate this common plane of polarisation so as to bring the direction of the electric field vector, E, perpendicular to the plane of the diagram; this ensures maximum contrast in the interference fringes.

A second converging lens or lens system L₂, in the form of a microscope objective, for example Olympus DA 10X, focusses the beams with the aid of a mirror system which is illustrated in Figure 2. The mirror system M is positioned against a transparent plate L₃ which is fixed in front of the microscope objective L₂; it consists of two flat downwardly tapering bodies M₁ and M₂ the inward facing walls of which are coated with a highly reflective layer, for example a layer of aluminium. The two beams emerging from the Wollaston prism W and polarising arrangement P₂, p₃ are indicated in Figure 2 by their principal rays B₁ and B₂. After emerging from the microscope objective L₂ (not shown in Figure 2) the two beams B₁ and B₂ pass through element L₃ towards mirror M₁ and M₂. The angle of incidence of the principal ray of each beam on its respective mirror is

67.5º. Element L₃ may be a glass or fused silica disk of convenient size, e.g. 20 mm diameter, which is fixed in front of the microscope objective L₂. Mirrors M₁ and M₂ bring the beams B₁ and B₂ to a focus at a point F about 0.1 mm below the bottom plane of the mirrors. The angle of intersection of the two beams is 90°. The distance between focus F and the remote surface of element L₃ is about 4 mm in this embodiment.

The Wollaston prism W operates by polarisation. The objective L₂ receives light from two apparent sources which are at a distance d apart, where d = 0.1 where 0 is the doubling angle of the Wollaston prism, typically about 2°, and 1 is the distance from the Wollaston prism to the pinhole, which will typically be about 200 mm. This separation is adjustable.

The halfwave plates P₁ and P₃ and the polariser P₂ are necessary to ensure that the virtual light sources are of equal intensity and that the interfering beams have the correct polarisation when they reach their focal point.

In use, a photoresist which is to be exposed is positioned in the plane of the focal point F. Typically, the resist is coated onto a flat circular disk substrate and the interference pattern is generated close to the outer perimeter of the disk; the disk is then rotated and translated radially during exposure so that a spiral track of fringes is produced. The disk carrying the photoresist will be located precisely with respect to the optical system in order to maintain the interferometer at a fixed height above the surface of the photoresist. This can be achieved by known techniques, for example by using air bearing or electronic servo techniques.

Claims

1. An interferometer which comprises: (1) a single, coherent light source; (2) a first converging lens positioned on the optical axis of said coherent light source; (3) a beam-splitting arrangement positioned on said optical axis and spaced from said first converging lens by a distance greater than the focal length of said lens; (4) a second converging lens positioned on said optical axis to receive and to focus the two beams emanating in use from the beam-splitting arrangement; and (5) a mirror arrangement positioned so that the beams focussed by said second converging lens impinge on the mirror system and so that the reflected beams are brought to intersect at a focal point and with a large angle between the principal rays of the two beams.

2. An interferometer as claimed in claim 1, wherein the beam-splitting arrangement comprises a Wollaston double image prism and a polarising arrangement.

3. An interferometer as claimed in claim 1 or 2, wherein said coherent light source is a laser generating light of wavelength of about 450nm or less.

4. An interferometer as claimed in claim 1, 2 or 3, wherein said first converging lens has a focal length of about 40 - 50mm and said second converging lens is a microscope objective lens.

5. An interferometer as claimed in claim 1, 2, 3 or 4, wherein the optical elements are arranged so that said reflected beams are brought to intersect at an angle of at least 45 degrees.

6. An interferometer as claimed in claim 5, wherein said angle of intersection is 90 degrees or greater.